Optical resonator with mirror structure suppressing higher order transverse modes
View Patent ↗An optical resonator including is designed is to degrade the ability of the resonator to support suppress higher order transverse spatial modes. The inventive optical resonator forces Higher higher order transverse modes to be fundamentally unstable in the inventive optical resonator, ultimately achieving ultimately to achieving single transverse mode resonator operation. Specifically, the bounded phase deflection mirror shape or intracavity lens profile is tailored to confine the fundamental mode while rendering the higher order modes unstable. This has application in MEMS/MOEMS optical resonator devices by suppressing the side modes and increasing the side mode suppression ratio (SMSR), as well as improving SMSR tolerance to device external alignment, for example. This also has application to achieving single transverse mode operation in laser resonators, such as in semiconductor vertical-cavity surface-emitting lasers (VCSEL).
1. An optical resonator comprising at least one optical cavity defined by at least two mirror structures in which at least one of the mirror structures has a mirror profile having a diameter and sag that are selected in combination with a length of the cavity to degrade a stability of transverse modes with mode numbers 4 and greater.
2. A resonator as claimed in claim 1 , wherein the length of the optical cavity is less than about 50 micrometers, the sag of the mirror profile is less than about 200 nanometers, and a full width at half maximum diameter of the mirror profile is less than 30 micrometers.
3. A resonator as claimed in claim 1 , wherein the length of the optical cavity is less than about 30 micrometers, the sag of the mirror profile is less than about 150 nanometers, and a full width at half maximum diameter of the mirror profile is less than 20 micrometers.
4. A resonator as claimed in claim 1 , wherein the length of the optical cavity is less than about 20 micrometers, the sag of the mirror profile is less than about 100 nanometers, and a full width at half maximum diameter of the mirror profile is less than 15 micrometers.
5. A resonator as claimed in claim 1 , wherein the sag of the mirror profile is less than about 150 nanometers.
6. A resonator as claimed in claim 1 , wherein the sag of the mirror profile is less than about 100 nanometers.
7. A resonator as claimed in claim 1 , wherein an optical distance between the mirror structures is tunable.
8. A resonator as claimed in claim 1 , wherein an optical distance between the mirror structures is tunable by out-of-plane deflection of one of the mirror structures.
9. A resonator as claimed in claim 1 , wherein a net profile of the mirror structures is concave in a center region surrounding an optical axis and flat and/or convex in an annular region surrounding the center region, and wherein the diameter and sag of the center region degrades the stability of transverse modes with mode numbers 4 and greater.
10. An optical resonator comprising at least one optical cavity defined by at least two mirror structures in which at least one of the mirror structures has a mirror profile having a diameter and sag, wherein the diameter and sag in combination with a length of the cavity degrade a stability of transverse modes with mode numbers 4 and greater.